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Figure 5.50. Outline of electroblotting experiment. Sample is electrophoresed in a polyacrylamide or agarose gel. It is then transferred to a membrane such as nitrocellulose by electrophoresis at right angles to the original direction. The membrane is then stained to identify particular sample components.

This situation is illustrated in Figure 4.18. It is clear from Figures 4.16, 4.17 and 4.18 that RL,b < RL,opt < RL,a and also Pout,b < Pout,max > Pout,a (4.35) (4.34)

P1: KOA WY050-04 WY050-Ulick-v4 September 19, 2004 11:4

where G(xf) is an arbitrary integrable complex function of a single variable. Then, the field pattern of equation (3.67) can be written as follows: h(0,f) =

[Mtext/Text/Angle]: Right-click and choose Mtext. In the In-Place Text Editor, press the End key on the keyboard and type a space, then type Typ. Click OK. Specify dimension line location or [Mtext/Text/Angle]: Pick a location for the dimension line.

(From left top, clockwise: DSA, PET, MR, MR, MR, CT)

FIGURE 7.6. Twyman-Green interferometer double passed to obtain modulated fringes. (From Hariharan and Sen, 1960a.)

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excited. These two modes are seen to be excited at frequencies in the vicinity of the fundamental resonant frequency (about 1.9 GHz) of the unloaded patch. For the impedance bandwidth de ned by 10-dB return loss, the case c = 40 provides an impedance bandwidth of 100 MHz, or about 5.2%, which is about 2.7 times that (36 MHz, or about 1.9%) of the corresponding unloaded circular microstrip antenna with a probe feed. Figure 7.55 shows the measured radiation patterns at resonance of the two resonant modes in the impedance bandwidth. Similar radiation characteristics have been observed for the two resonant modes, and cross-polarized radiation is seen below 20 dB. Figure 7.56 shows the measured antenna gain in the broadside direction. The antenna-gain variation in the impedance bandwidth is within 3 dBi, and a lower antenna gain is observed near the center frequency or at frequencies between the two resonant modes. It is expected that, by exciting the two resonant modes at frequencies closer to each other, the antenna gain near the center frequency can be enhanced, and the antenna-gain variation within the impedance bandwidth can be further reduced. 7.5.3 Design with a Bow-Tie Patch Figure 7.57 shows the geometry of a probe-fed bow-tie microstrip antenna with an inserted integrated reactive loading for bandwidth enhancement [28]. The dimensions of the bow-tie patch with integrated reactive loading are given in the gure. The bow-tie patch has a are angle and a width 24.9 mm, and the length between its two radiating edges is xed to be 37.3 mm. To integrate the cascaded microstrip-line sections to provide reactive loading, a rectangular notch of dimensions

This is the number of specifications in the second line of the definition, including the mandatory 0 at the end. You must use uppercase for the shape name. This is the name you use with the SHAPE command. This is a code that defines the actual shape. Each specification code defines a part of the shape, such as a line segment or an arc. Together, all of the specifications draw the shape. The definition must end with a 0.

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